Fredholm-Type Boundary Integral Expression of Forced Convection Heat Transfer and Its Application to Convection-Conduction Conjugated Heat Transfer Problem
We propose a Fredholm-type boundary integral expression of the forced convection heat transfer coefficient from an object. When the Fredholm's kernel function is obtained by a numerical simulation of the forced convection field, it is possible to predict the local heat transfer coefficient from...
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Veröffentlicht in: | JSME International Journal Series B Fluids and Thermal Engineering 1997/08/15, Vol.40(3), pp.447-453 |
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creator | MOMOSE, Kazunari SASOH, Kiyoshi KIMOTO, Hideo |
description | We propose a Fredholm-type boundary integral expression of the forced convection heat transfer coefficient from an object. When the Fredholm's kernel function is obtained by a numerical simulation of the forced convection field, it is possible to predict the local heat transfer coefficient from the object with arbitrary surface temperature distributions. Moreover, this expression can be easily applied to the boundary element method(BEM)as a boundary condition of fourth kind, and then the convection-conduction conjugated heat transfer problem can be formulated as a heat conduction problem. Some examples demonstrate the usefulness of the proposed expression. |
doi_str_mv | 10.1299/jsmeb.40.447 |
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When the Fredholm's kernel function is obtained by a numerical simulation of the forced convection field, it is possible to predict the local heat transfer coefficient from the object with arbitrary surface temperature distributions. Moreover, this expression can be easily applied to the boundary element method(BEM)as a boundary condition of fourth kind, and then the convection-conduction conjugated heat transfer problem can be formulated as a heat conduction problem. 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When the Fredholm's kernel function is obtained by a numerical simulation of the forced convection field, it is possible to predict the local heat transfer coefficient from the object with arbitrary surface temperature distributions. Moreover, this expression can be easily applied to the boundary element method(BEM)as a boundary condition of fourth kind, and then the convection-conduction conjugated heat transfer problem can be formulated as a heat conduction problem. Some examples demonstrate the usefulness of the proposed expression.</description><subject>Boundary Element Method</subject><subject>Boundary Integral</subject><subject>Conjugated Problem</subject><subject>Convective and constrained heat transfer</subject><subject>Exact sciences and technology</subject><subject>Forced Convection</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Heat Conduction</subject><subject>Heat transfer</subject><subject>Heat Transfer Coefficent</subject><subject>Natural convection</subject><subject>Physics</subject><issn>1340-8054</issn><issn>1347-5371</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1997</creationdate><recordtype>article</recordtype><recordid>eNpVkFFv2yAUha1pk9Z1e9sPQNoe5xQMGPzYRckaqdL2kD0jDJfUlmM8wFP7W_ZnR-Iu6l7giPPdc8Upio8Er0jVNDd9PEK7YnjFmHhVXBHKRMmpIK_PGpcSc_a2eBdjjzGlvG6uij_bAPbBD8dy_zQB-urn0erwhHZjgkPQA9o8TgFi7PyIvENbHwxYtPbjbzDp9HgHOqF90GN0EJAeLdqliG6naeiMPhPJv-DLLO28jGbZzwedcuD_KT-Cbwc4vi_eOD1E-PB8Xxc_t5v9-q68__5tt769Lw0XPJUVNq5qjWWYU9li1gC0TAqnjXPScRC2FhJbw7BrrKt0rSWpDaGGW8i2ptfFpyV3Cv7XDDGp3s9hzCsVYbXgFRFSZurLQpngYwzg1BS6Y-5KEaxO9atz_YphlevP-OfnUB2NHlz-m-niZaaSpCKMZGyzYH1M-gAXX4fUmQGWTNI09JT772Di4psHHRSM9C_1faJ-</recordid><startdate>1997</startdate><enddate>1997</enddate><creator>MOMOSE, Kazunari</creator><creator>SASOH, Kiyoshi</creator><creator>KIMOTO, Hideo</creator><general>The Japan Society of Mechanical Engineers</general><general>Japan Society of Mechanical Engineers</general><general>Japan Science and Technology Agency</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>1997</creationdate><title>Fredholm-Type Boundary Integral Expression of Forced Convection Heat Transfer and Its Application to Convection-Conduction Conjugated Heat Transfer Problem</title><author>MOMOSE, Kazunari ; SASOH, Kiyoshi ; KIMOTO, Hideo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c575t-20cf2bcd40538b049eeb487facff8f5e7d6780dc40f9df2a6a816c13c5def5ea3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1997</creationdate><topic>Boundary Element Method</topic><topic>Boundary Integral</topic><topic>Conjugated Problem</topic><topic>Convective and constrained heat transfer</topic><topic>Exact sciences and technology</topic><topic>Forced Convection</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Heat Conduction</topic><topic>Heat transfer</topic><topic>Heat Transfer Coefficent</topic><topic>Natural convection</topic><topic>Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>MOMOSE, Kazunari</creatorcontrib><creatorcontrib>SASOH, Kiyoshi</creatorcontrib><creatorcontrib>KIMOTO, Hideo</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>JSME International Journal Series B Fluids and Thermal Engineering</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>MOMOSE, Kazunari</au><au>SASOH, Kiyoshi</au><au>KIMOTO, Hideo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Fredholm-Type Boundary Integral Expression of Forced Convection Heat Transfer and Its Application to Convection-Conduction Conjugated Heat Transfer Problem</atitle><jtitle>JSME International Journal Series B Fluids and Thermal Engineering</jtitle><date>1997</date><risdate>1997</risdate><volume>40</volume><issue>3</issue><spage>447</spage><epage>453</epage><pages>447-453</pages><issn>1340-8054</issn><eissn>1347-5371</eissn><abstract>We propose a Fredholm-type boundary integral expression of the forced convection heat transfer coefficient from an object. When the Fredholm's kernel function is obtained by a numerical simulation of the forced convection field, it is possible to predict the local heat transfer coefficient from the object with arbitrary surface temperature distributions. Moreover, this expression can be easily applied to the boundary element method(BEM)as a boundary condition of fourth kind, and then the convection-conduction conjugated heat transfer problem can be formulated as a heat conduction problem. Some examples demonstrate the usefulness of the proposed expression.</abstract><cop>Tokyo</cop><pub>The Japan Society of Mechanical Engineers</pub><doi>10.1299/jsmeb.40.447</doi><tpages>7</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Boundary Element Method Boundary Integral Conjugated Problem Convective and constrained heat transfer Exact sciences and technology Forced Convection Fundamental areas of phenomenology (including applications) Heat Conduction Heat transfer Heat Transfer Coefficent Natural convection Physics |
title | Fredholm-Type Boundary Integral Expression of Forced Convection Heat Transfer and Its Application to Convection-Conduction Conjugated Heat Transfer Problem |
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